Abstract

Abstract A correction of CTOD for constraint loss in large-scale yielding conditions is made on the basis of the Weibull stress fracture criterion that eliminates an excessive conservatism in the conventional fracture assessment and material fracture toughness requirement. A CTOD ratio β = δ3P / δWP (<1) is proposed, where δWP is the CTOD of a wide plate component and δ3P is an equivalent CTOD of the fracture toughness specimen at which the toughness specimen gives a compatible Weibull stress with the wide plate. The CTOD ratio β is decreased to a large extent after full yielding of the wide plate component, which is more significant for a high yield ratio YR and a deep surface crack in the wide plate. The Weibull modulus m exerts a marginal influence on β. A case study is presented on the application of the CTOD ratio β to the fracture performance assessment of full-scale column-to-beam connections subjected to cyclic and dynamic loading.

Highlights

  • The fracture mechanics approach to structural design and material selection relies on the stress intensity factor K, crack tip opening displacement (CTOD, δ) and J integral as the controlling parameters for stress fields ahead of a crack

  • In order to overcome limitations of the toughness scaling model (TSM), a modified toughness scaling with the Weibull stress was developed [7, 8], which requires the attainment of a specified Weibull stress to cause cleavage fracture at the same probability in different specimen geometry

  • This paper presented the CTOD toughness scaling between structural components and fracture toughness specimens

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Summary

INTRODUCTION

The fracture mechanics approach to structural design and material selection relies on the stress intensity factor K, crack tip opening displacement (CTOD, δ) and J integral as the controlling parameters for stress fields ahead of a crack. In large-scale yielding conditions, the actual stress fields deviate from the K- and Jcontrolled fields and depend significantly on the crack size and geometry of specimens employed This is due to the constraint effect on the crack-tip plasticity. A loss of constraint resulting from large-scale yielding relaxes the stress elevation for notched-tension panels and shallow-notch specimens, while deep-notch bend and compact specimens maintain a high level of crack tip constraint. Such constraint loss leads to an apparently increased fracture resistance Kc , δc and Jc for the former configurations. The CTOD values were calculated according to BS7448 for the compact and deep-notch bend

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CONCLUSIONS
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